Is the "op" lattice ##\mathscr{L_H}^\perp## also atomistic....?

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The "op" lattice ##\mathscr{L_H}^\perp##, derived from the lattice of subspaces of Hilbert space ##\mathscr{H}##, is confirmed to be atomistic and possesses the covering property. The orthocomplements of pure states in ##\mathscr{L_H}## serve as the atoms in ##\mathscr{L_H}^\perp##. A proof is established by demonstrating that for any two subspaces ##q_1, q_2 \in \mathscr{L_H}^\perp##, if ##q_1 \leq p^\perp \leq q_2##, then either ##q_1 = 0## or ##q_2 = p^\perp##. This conclusion aligns with the atomicity of the original lattice ##\mathscr{L_H}##.

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Is the "op" lattice of subspaces of a Hilbert space also atomistic with the covering property?
Let ##\mathscr{L_H}## be the usual lattice of subspaces of Hilbert space ##\mathscr{H}##, where for ##p,q\in\mathscr{H}## we write ##p\leq q## iff ##p## is a subspace of ##q##. Then, as discussed by, e.g., Beltrametti&Cassinelli https://books.google.com/books?id=yWoq_MRKAgcC&pg=PA98, this lattice is atomistic with the covering property. That is, enormously briefly, ##0## is the weakest element, i.e., ##\forall q\in\mathscr{H}: 0\leq q##, and pure states ##p## (one-dimensional subspaces) are "atoms" with the covering property, i.e., ##\forall q\in\mathscr{H}: 0\leq q\leq p\Longrightarrow 0=q\mbox{ .or. }q=p##.

Now consider the "op" lattice ##\mathscr{L_H}^\perp## where ##q\leq p## in ##\mathscr{L_H}## means ##p\leq q## in ##\mathscr{L_H}^\perp##. Then ##0^\perp=\mathscr{H}\in \mathscr{L_H}^\perp## is the weakest element. And can we say that (a) the orthocomplements of pure states are the atoms of ##\mathscr{L_H}^\perp##, and that (b) they also possesses the corresponding covering property with respect to this lattice? And can you prove it, or even better (and presumably easier) cite a proof? Note that by "prove", you can assume it's true for ##\mathscr{L_H}##, and only need to prove it's then also true for ##\mathscr{L_H}^\perp##.

P.S. Another discussion of atomistic lattices with the covering property is in Section 4.2.5 (pages 4-10 and 4-11) of https://arxiv.org/abs/1211.5627
 
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.Yes, it is true that orthocomplements of pure states are the atoms of ##\mathscr{L_H}^\perp##, and they also possess the covering property with respect to this lattice. To prove this, we will first show that the orthocomplements of pure states are the atoms of ##\mathscr{L_H}^\perp##, and then show that they have the covering property.First, we will show that the orthocomplements of pure states are the atoms of ##\mathscr{L_H}^\perp##. Suppose that ##p \in \mathscr{L_H}## is a pure state, and let ##p^\perp \in \mathscr{L_H}^\perp## be its orthocomplement. We want to show that ##p^\perp## is an atom in ##\mathscr{L_H}^\perp##. That is, we need to show that for any two subspaces ##q_1, q_2 \in \mathscr{L_H}^\perp## such that ##q_1 \leq p^\perp \leq q_2##, either ##q_1 =0## or ##q_2 = p^\perp##.Let ##q_1, q_2 \in \mathscr{L_H}^\perp## be two subspaces such that ##q_1 \leq p^\perp \leq q_2##. By definition, this means that ##p \leq q_1^\perp \leq p^\perp \leq q_2^\perp##. Now, since ##p## is a pure state, it follows from the atomicity of ##\mathscr{L_H}## that either ##q_1^\perp =0## or ##q_2^\perp = p##. This implies that either ##q_1 =0## or ##q_2 = p^\perp##, as desired. Thus, we have shown that the orthocomplements of pure states are the atoms of ##\mathscr{L_H}^
 

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